Imaging lens

ABSTRACT

An imaging lens includes a first lens group having positive refractive power; a second lens group having negative refractive power; and a third lens group having negative refractive power, arranged in this order from an object side to an image plane side. The first lens group includes a first lens having positive refractive power, a second lens having negative refractive power, and a third lens having positive refractive power. The second lens group includes a fourth lens and a fifth lens. The third lens group includes a sixth lens having positive refractive power and a seventh lens having negative refractive power. The first to third lenses and the sixth to seventh lenses have specific Abbe&#39;s numbers.

BACKGROUND OF THE INVENTION AND RELATED ART STATEMENT

The present invention relates to an imaging lens for forming an image ofan object on an imaging element such as a CCD sensor and a CMOS sensor.In particular, the present invention relates to an imaging lens suitableto be mounted in a relatively small camera such as a camera to be builtin a portable device including a cellular phone and a portableinformational terminal, a digital still camera, a security camera, avehicle onboard camera, and a network camera.

In these years, in place of cellular phones intended mainly for makingphone calls, so-called smartphones, i.e., cellular phones with functionsof portable information terminals (PDAs) and/or personal computers, havebeen more widely used. Since the smartphones generally are highlyfunctional as opposed to the cellular phones, it is possible to useimages taken by a camera thereof in various applications.

Generally speaking, product groups of cellular phones and smartphonesare often composed according to specifications for beginners to advancedusers. Among them, an imaging lens to be mounted in the productsdesigned for advanced users is required to have a high-resolution lensconfiguration so as to be also applicable to a high pixel count imagingelement developed in these years.

As a method of attaining a high-resolution imaging lens, there is amethod of increasing the number of lenses that compose the imaging lens.However, the increase of the number of lenses easily causes an increasein the size of the imaging lens, so that the lens configuration having alarge number of lenses is disadvantageous to be mounted in a small-sizedcamera such as the above-described cellular phones and smartphones. Forthis reason, the imaging lens has been developed so as to restrain thenumber of lenses as small as possible. However, with rapid advancementin these days for achieving a higher pixel count of an imaging element,an imaging lens has been developed so as to attain higher resolutionrather than a shorter total track length of the imaging lens. As anexample, there is an advent of a camera unit formed to be able to obtainan image that is equivalent to that of a digital still camera byattaching the camera unit to a cellular phone or a smartphone, which isdifferent from a conventional camera unit containing an imaging lens andan imaging element to be mounted inside a cellular phone or asmartphone.

In case of a lens configuration composed of seven lenses, since thenumber of lenses that compose an imaging lens is large, it is somewhatdisadvantageous for downsizing of the imaging lens. However, since thereis high flexibility in designing, it has potential of attainingsatisfactory correction of aberrations and downsizing in a balancedmanner. For example, as a lens configuration composed of seven lenses,an imaging lens described in Patent Reference has been known.

Patent Reference: Japanese Patent Application Publication No.2012-155223

The imaging lens described in Patent Reference includes a first lenshaving a biconvex shape; a second lens that is joined to the first lensand has a biconcave shape; a third lens that is negative and has a shapeof a meniscus lens directing a convex surface thereof to an object side;a fourth lens that is positive and has a shape of a meniscus lensdirecting a concave surface thereof to the object side; a fifth lensthat is negative and has a convex surface directing to the object side;a sixth lens having a biconvex shape; and a seventh lens having abiconcave shape, arranged in the order from the object side.

According to the imaging lens disclosed in Patent Reference, whenrestraining a ratio between a focal length of a first lens groupcomposed of the lenses from the first lens to the fourth lens to a focallength of a second lens group composed of the lenses from the fifth lensto the seventh lens in a certain range, it is possible to attaindownsizing of the imaging lens and satisfactory correction ofaberrations.

The imaging lens described in Patent Reference has a small size, butaberrations on an image plane are not sufficiently corrected andespecially distortion is relatively large. Therefore, there is a limitby itself in achieving a high-resolution imaging lens. According to thelens configuration described in Patent Reference, it is difficult toachieve satisfactory aberration correction while downsizing the imaginglens.

Here, such an issue is not a problem specific to the imaging lens to bemounted in cellular phones and smartphones. Rather, it is a commonproblem even for an imaging lens to be mounted in a relatively smallcamera such as digital still cameras, portable information terminals,security cameras, vehicle onboard cameras, and network cameras.

In view of the above-described problems in conventional techniques, anobject of the present invention is to provide an imaging lens that canattain downsizing thereof and satisfactory aberration correction.

Further objects and advantages of the present invention will be apparentfrom the following description of the present invention.

SUMMARY OF THE PRESENT INVENTION

In order to attain the objects described above, according to a firstaspect of the present invention, an imaging lens includes a first lensgroup having positive refractive power, a second lens group havingnegative refractive power, and a third lens group having negativerefractive power, arranged in the order from an object side to an imageplane side. The first lens group includes a first lens having positiverefractive power, a second lens having negative refractive power, and athird lens having positive refractive power. The second lens groupincludes a fourth lens and a fifth lens. The third lens group includes asixth lens having positive refractive power and a seventh lens havingnegative refractive power.

According to the first aspect of the present invention, when the firstlens has an Abbe's number νd1, the second lens has an Abbe's number νd2,the third lens has an Abbe's number νd3, the sixth lens has an Abbe'snumber νd6, and the seventh lens has an Abbe's number νd7, the imaginglens of the present invention satisfies the following conditionalexpressions (1) to (5):40<νd1<75  (1)20<νd2<35  (2)40<νd3<75  (3)40<νd6<75  (4)20<νd7<35  (5)

According to the first aspect of the present invention, in the imaginglens, there are arranged the first lens group having positive refractivepower and the second lens group having negative refractive power, sothat a chromatic aberration is satisfactorily corrected in those lensgroups. Therefore, according to the imaging lens of the presentinvention, it is possible to satisfactorily correct aberrations,especially the chromatic aberration, and obtain satisfactoryimage-forming performance, which is necessary for a high-resolutionimaging lens. In addition, according to the imaging lens of the presentinvention, since the third lens group has negative refractive power, itis possible to suitably downsize the imaging lens.

The first lens group includes three lenses, refractive powers of whichare arranged in the order of positive, negative, and positive. Thosethree lenses are made from lens materials that satisfy the conditionalexpressions (1) to (3), respectively. With the order of refractivepowers of the respective lenses and the arrangement of the Abbe'snumbers, in the first lens group, it is possible to suitably restraingeneration of the chromatic aberration and satisfactorily correct thechromatic aberration if generated.

Furthermore, according to the first aspect of the present invention, inthe imaging lens, the third lens group includes two lenses, which arepositive and negative lenses and are made to be a combination of a lensmade of a low-dispersion lens material and a lens made of ahigh-dispersion lens material, so as to satisfy the above-describedconditional expressions (4) and (5). For this reason, it is possible tomore satisfactorily correct aberrations generated in the first lensgroup and the second lens group, especially the chromatic aberration.Generally speaking, in order to attain a high-resolution imaging lens,it is necessary to satisfactorily correct aberrations, especially thechromatic aberration.

According to the first aspect of the present invention, in the imaginglens, with the order of refractive powers of the respective lens groupsof the first lens group to the third lens group, the order of refractivepowers and the arrangement of Abbe's numbers of the three lenses thatcompose the first lens group, and the order of refractive powers and thearrangement of Abbe's numbers of the two lenses that compose the thirdlens group, it is possible to more satisfactorily correct the chromaticaberration than conventional imaging lenses.

According to a second aspect of the present invention, when the fourthlens has negative refractive power, the fifth lens has negativerefractive power, the fourth lens has an Abbe's number νd4, and thefifth lens has an Abbe's number νd5, the imaging lens having theabove-described configuration preferably satisfies the followingconditional expressions (6) and (7):20<νd4<35  (6)20<νd5<35  (7)

According to the second aspect of the present invention, the second lensof the first lens group and the seventh lens of the third lens grouprespectively have negative refractive power and are respectively formedof high-dispersion materials as indicated in the above conditionalexpressions (2) and (5). According to the imaging lens of the presentinvention, the second lens group disposed between the first lens groupand the third lens group has negative refractive power. The respectivelenses that compose the second lens group are made of high-dispersionmaterials as indicated in the conditional expressions (6) and (7).

Therefore, according to the second aspect of the present invention, itis possible to more satisfactorily correct the chromatic aberration.Here, the second lens group is composed of two lenses, so that therespective lenses can have smaller refractive powers than when thesecond lens group is composed of one lens, and thereby it is easy tocorrect aberrations.

According to a third aspect of the present invention, in the imaginglens having the above-described configuration, the sixth lens and theseventh lens are preferably formed as aspheric shapes such that positiverefractive powers thereof are increasing toward the lens peripheriesthereof from an optical axis.

According to the third aspect of the present invention, the sixth lensand the seventh lens that compose the third lens group are formed inshapes such that positive refractive powers thereof become strong towardthe lens peripheries thereof from the optical axis. With theconfiguration, it is possible to satisfactorily correct an off-axischromatic aberration of magnification as well as an axial chromaticaberration, and it is also possible to suitably restrain an incidentangle of a light beam emitted from the imaging lens to an imagingelement. As is well known, in case of an imaging element of a CCDsensor, a CMOS sensor or the like, a range of incident angle of a lightbeam that can be taken in a sensor (so-called “chief ray angle (CRA)”)is set in advance. Since the sixth lens and the seventh lens have theabove-described lens shapes, it is possible to suitably restrain theincident angle of a light beam emitted from the imaging lens to an imageplane within the range of CRA. Therefore, it is possible to suitablyrestrain generation of shading, which is a phenomenon of becoming darkon the image periphery.

According to a fourth aspect of the present invention, when the wholelens system has a focal length f, and a distance on an optical axisbetween the fifth lens and the sixth lens is D56, the imaging lenshaving the above-described configuration preferably satisfies thefollowing conditional expression (8):0.02<D56/f<0.15  (8)

When the imaging lens satisfies the conditional expression (8), it ispossible to satisfactorily correct the chromatic aberration and adistortion, while reducing the size of the imaging lens. In addition,when the imaging lens satisfies the conditional expression (8), it isalso possible to restrain the incident angle of a light beam emittedfrom the imaging lens to the imaging element within the range of CRA.When the value exceeds the upper limit of “0.15”, it is easy to restrainthe incident angle to the imaging element within the range of CRA, andit is advantageous for correction of the chromatic aberration. However,since a back focal length is short, it is difficult to secure space fordisposing an insert such as an infrared cut-off filter. Moreover, in theastigmatism, a sagittal image surface curves to the object side, so thatit is difficult to obtain satisfactory image-forming performance.

On the other hand, when the value is below the lower limit of “0.02”,although it is advantageous for correction of the distortion, anastigmatic difference increases. Furthermore, the chromatic aberrationof magnification is excessively corrected (an image-forming point at ashort wavelength moves in a direction away from the optical axisrelative to an image-forming point at a reference wavelength), so thatit is difficult to obtain satisfactory image-forming performance.Moreover, in this case, it is also difficult to restrain the incidentangle to the imaging element within the range of CRA.

According to a fifth aspect of the present invention, when the wholelens system has a focal length f and a composite focal length from thefirst lens to the third lens is f123, the imaging lens having theabove-described configuration preferably satisfies the followingconditional expression (9):0.6<f123/f<1.2  (9)

When the imaging lens satisfies the conditional expression (9), it ispossible to restrain astigmatism and the chromatic aberration withinsatisfactory ranges in a balanced manner, while reducing the size of theimaging lens. When the value exceeds the upper limit of “1.2”, thepositive refractive power of the first lens group is weak relative tothe refractive power of the whole lens system. Therefore, although it isadvantageous for correcting the chromatic aberration and securing theback focal length, it is difficult to attain downsizing of the imaginglens. In addition, in the astigmatism, a tangential image surface curvesto the image plane side and the astigmatic difference increases, so thatit is difficult to obtain satisfactory image-forming performance.

On the other hand, when the value is below the lower limit of “0.6”, thepositive refractive power of the first lens group is strong relative tothe refractive power of the whole lens system, so that the negativerefractive power of the second lens in the first lens group isrelatively weak. For this reason, although it is advantageous fordownsizing of the imaging lens and correction of the astigmatism, it isdifficult to secure the back focal length. Moreover, the axial chromaticaberration is insufficiently corrected (a focal position at a shortwavelength moves to the object side relative to a focal position at areference wavelength), and the chromatic aberration of magnification isinsufficiently corrected (an image-forming point at a short wavelengthmoves in a direction close to the optical axis relative to animage-forming point at a reference wavelength). Therefore, it isdifficult to obtain satisfactory image-forming performance.

According to a sixth aspect of the present invention, when the wholelens system has a focal length f and a composite focal length of thesixth lens and the seventh lens is f67, the imaging lens having theabove-described configuration preferably satisfies the followingconditional expression (10):−15<f67/f<−1.5  (10)

When the imaging lens satisfies the conditional expression (10), it ispossible to restrain the astigmatism, the distortion, and the chromaticaberration within satisfactory ranges in a balanced manner. When thevalue exceeds the upper limit of “−1.5”, it is advantageous forcorrecting the chromatic aberration of magnification. However, thedistortion increases in a plus direction and the astigmatic differenceincreases at image periphery, so that it is difficult to obtainsatisfactory image-forming performance.

On the other hand, when the value is below the lower limit of “−15”,although it is advantageous for correction of the distortion andcorrection of the axial chromatic aberration, the astigmatic differenceincreases and the chromatic aberration of magnification isinsufficiently corrected for the off-axis light beams, so that it isdifficult to obtain satisfactory image-forming performance.

According to a seventh aspect of the present invention, in order to moresatisfactorily correct the astigmatism, the distortion, and thechromatic aberration, the imaging lens having the above-describedconfiguration preferably satisfies the following conditional expression(10A):−12<f67/f<−1.5  (10A)

According to an eighth aspect of the present invention, when the sixthlens has a focal length f6 and a composite focal length of the fourthlens and the fifth lens is f45, the imaging lens having theabove-described configuration preferably satisfies the followingconditional expression (11):−2<f45/f6<−0.1  (11)

When the imaging lens satisfies the conditional expression (11), it ispossible to satisfactorily correct the chromatic aberration, thedistortion, and the astigmatism, while restraining the incident angle ofa light beam emitted from the imaging lens to the imaging element withinthe range of CRA. When the value exceeds the upper limit of “−0.1”, thepositive refractive power of the sixth lens is weak relative to therefractive power of the second lens group, so that it is easy to securethe back focal length. However, the distortion increases in the plusdirection and the chromatic aberration of magnification is excessivelycorrected for the off-axis light beams, so that it is difficult toobtain satisfactory image-forming performance.

On the other hand, when the value is below the lower limit of “−2”,although it is easy to restrain the incident angle to the imagingelement within the range of CRA, the distortion increases in the minusdirection and the chromatic aberration of magnification isinsufficiently corrected for the off-axis light beams. In addition, theastigmatic difference increases. Therefore, it is difficult to obtainsatisfactory image-forming performance.

According to a ninth aspect of the present invention, when the wholelens system has a focal length f and the fourth lens has a focal lengthf4, the imaging lens having the above-described configuration preferablysatisfies the following conditional expression (12):−15<f4/f<−3  (12)

When the imaging lens satisfies the conditional expression (12), it ispossible to satisfactorily correct a spherical aberration, the chromaticaberration, and a field curvature. When the value exceeds the upperlimit of “−3”, the negative refractive power of the fourth lens isstrong relative to the refractive power of the whole lens system, sothat it is advantageous for correction of the axial chromaticaberration, the chromatic aberration of magnification, and the sphericalaberration. However, since the periphery of the image-forming surfacecurves to the object side, it is difficult to satisfactorily correct thefield curvature.

On the other hand, when the value is below the lower limit of “−15”, theaxial chromatic aberration and the chromatic aberration of magnificationare both insufficiently corrected, and the periphery of theimage-forming surface curves to the image plane side, so that it isdifficult to satisfactorily correct the field curvature. Therefore, ineither case, it is difficult to obtain satisfactory image-formingperformance.

In order to more satisfactorily correct the spherical aberration, thechromatic aberration, and the field curvature, according to a tenthaspect of the present invention, the imaging lens having theabove-described configuration preferably satisfies the followingconditional expression (12A):−12<f4/f<−3  (12A)

According to an eleventh aspect of the present invention, when the wholelens system has a focal length f and the first lens has a focal lengthf1, the imaging lens having the above-described configuration preferablysatisfies the following conditional expression (13):0.5<f1/f<2.0  (13)

When the imaging lens satisfies the conditional expression (13), it ispossible to restrain the astigmatism, the chromatic aberration, and thespherical aberration within the preferred ranges in a balanced manner,while downsizing the imaging lens. When the value exceeds the upperlimit of “2.0”, the first lens has weak refractive power relative to therefractive power of the whole lens system. Therefore, although it iseasy to secure the back focal length, it is difficult to attaindownsizing of the imaging lens. In addition, in the astigmatism, thesagittal image surface curves to the object side, and the image-formingsurface curves to the object side, so that it is difficult to obtainsatisfactory image-forming performance.

On the other hand, when the value is below the lower limit of “0.5”,although it is advantageous for downsizing of the imaging lens, it isdifficult to secure the back focal length. Moreover, in the astigmatism,the tangential image surface curves to the image plane side, and theastigmatic difference increases. In addition, the spherical aberrationincreases. Therefore, it is difficult to obtain satisfactoryimage-forming performance.

According to a twelfth aspect of the present invention, when the firstlens has a focal length f1, the second lens has a focal length f2, theimaging lens having the above-described configuration preferablysatisfies the following conditional expression (14):−4<f2/f<−0.5  (14)

When the imaging lens satisfies the conditional expression (14), it ispossible to restrain the spherical aberration, the astigmatism, thefield curvature, and the chromatic aberration within preferred ranges ina balanced manner. When the value exceeds the upper limit of “−0.5”, thenegative refractive power of the second lens is strong relative to therefractive power of the whole lens system. Therefore, although it isadvantageous for correction of the axial chromatic aberration and thespherical aberration, the astigmatic difference increases. Accordingly,it is difficult to obtain satisfactory image-forming performance.

On the other hand, when the value is below the lower limit of “−4, therefractive power of the second lens is weak relative to the refractivepower of the whole lens system, so that the axial chromatic aberrationand the chromatic aberration of magnification are both insufficientlycorrected. In addition, the image-forming surface curves to the objectside. Therefore, it is difficult to obtain satisfactory image-formingperformance.

According to a thirteenth aspect of the present invention, when thefirst lens has a focal length f1 and the third lens has a focal lengthf3, the imaging lens having the above-described configuration preferablysatisfies the following conditional expression (15):1<f3/f<4  (15)

When the imaging lens satisfies the conditional expression (15), it ispossible to satisfactorily correct the chromatic aberration and thespherical aberration. When the value exceeds the upper limit of “4”, therefractive power of the third lens is weak relative to the refractivepower of the whole lens system. Therefore, the axial chromaticaberration is insufficiently corrected, and it is difficult to correctthe spherical aberration. For this reason, it is difficult to obtainsatisfactory image-forming performance.

On the other hand, when the value is below the lower limit of “1”, it isadvantageous for correction of the spherical aberration and correctionof the chromatic aberration. However, the chromatic aberration of thesagittal light beam at image periphery increases. Therefore, it isdifficult to obtain satisfactory image-forming performance.

According to the imaging lens of the present invention, it is possibleto provide a small-sized imaging lens, which is especially suitable formounting in a small-sized camera, while having satisfactorily correctedaberrations and high resolution.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a sectional view of a schematic configuration of an imaginglens in Numerical Data Example 1 according to an embodiment of thepresent invention;

FIG. 2 is an aberration diagram showing a lateral aberration of theimaging lens of FIG. 1;

FIG. 3 is an aberration diagram showing a spherical aberration,astigmatism, and a distortion of the imaging lens of FIG. 1;

FIG. 4 shows a sectional view of a schematic configuration of an imaginglens in Numerical Data Example 2 according to the embodiment of thepresent invention;

FIG. 5 is an aberration diagram showing a lateral aberration of theimaging lens of FIG. 4;

FIG. 6 is an aberration diagram showing a spherical aberration,astigmatism, and a distortion of the imaging lens of FIG. 4;

FIG. 7 shows a sectional view of a schematic configuration of an imaginglens in Numerical Data Example 3 according to the embodiment of thepresent invention;

FIG. 8 is an aberration diagram showing a lateral aberration of theimaging lens of FIG. 7;

FIG. 9 is an aberration diagram showing a spherical aberration,astigmatism, and a distortion of the imaging lens of FIG. 7;

FIG. 10 shows a sectional view of a schematic configuration of animaging lens in Numerical Data Example 4 according to the embodiment ofthe present invention;

FIG. 11 is an aberration diagram showing a lateral aberration of theimaging lens of FIG. 10;

FIG. 12 is an aberration diagram showing a spherical aberration,astigmatism, and a distortion of the imaging lens of FIG. 10;

FIG. 13 shows a sectional view of a schematic configuration of animaging lens in Numerical Data Example 5 according to the embodiment ofthe present invention;

FIG. 14 is an aberration diagram showing a lateral aberration of theimaging lens of FIG. 13;

FIG. 15 is an aberration diagram showing a spherical aberration,astigmatism, and a distortion of the imaging lens of FIG. 13;

FIG. 16 shows a sectional view of a schematic configuration of animaging lens in Numerical Data Example 6 according to the embodiment ofthe present invention;

FIG. 17 is an aberration diagram showing a lateral aberration of theimaging lens of FIG. 16; and

FIG. 18 is an aberration diagram showing a spherical aberration,astigmatism, and a distortion of the imaging lens of FIG. 16.

DETAILED DESCRIPTION OF PREFERRED EMBODIMENTS

Hereunder, referring to the accompanying drawings, an embodiment of thepresent invention will be fully described.

FIGS. 1, 4, 7, 10, 13, and 16 are schematic sectional views of theimaging lenses in Numerical Data Examples 1 to 6 according to theembodiment, respectively. Since a basic lens configuration is the sameamong those Numerical Data Examples, the lens configuration of theembodiment will be described with reference to the illustrativesectional view of Numerical Data Example 1.

As shown in FIG. 1, the imaging lens of the embodiment includes a firstlens group G1 having positive refractive power, a second lens group G2having negative refractive power, and a third lens group G3 havingnegative refractive power, arranged in the order from an object side toan image plane side. Between the third lens group G3 and an image planeIM of an imaging element, there is provided a filter 10. The filter 10is omissible.

The first lens group G1 includes a first lens L1 having positiverefractive power, an aperture stop ST, a second lens L2 having negativerefractive power, and a third lens L3 having positive refractive power,arranged in the order from the object side. The first lens L1 is formedin a shape such that a curvature radius r1 of an object-side surfacethereof and a curvature radius r2 of an image plane-side surface thereofare both positive, so as to have a shape of a meniscus lens directing aconvex surface to the object side near an optical axis X. The shape ofthe first lens L1 is not limited to the one in Numerical Data Example 1.The first lens L1 can be formed in any shape as long as the curvatureradius r1 of the object-side surface thereof is positive. The first lensL1 can be formed in a shape such that the curvature radius r2 of theimage plane-side surface thereof is negative, i.e., a shape of abiconvex lens near the optical axis X. Numerical Data Example 3 is anexample, in which the first lens L1 has a shape of a biconvex lens nearthe optical axis X. Here, according to the imaging lens of theembodiment, there is provided an aperture stop ST on the imageplane-side surface of the first lens L1.

The second lens L2 is formed in a shape such that a curvature radius r3of an object-side surface thereof and a curvature radius r4 of an imageplane-side surface thereof are both positive, so as to have a shape of ameniscus lens directing a convex surface to the object side near theoptical axis X. Here, the shape of the second lens L2 is not limited tothe one in Numerical Data Example 1. The second lens L2 can be formed inany shape as long as the curvature radius r4 of the image plane-sidesurface thereof is positive. The second lens L2 can also be formed in ashape such that the curvature radius r3 of the object-side surfacethereof is negative, i.e., a shape of a biconcave lens near the opticalaxis X.

The third lens L3 is formed in a shape such that a curvature radius r5of an object-side surface thereof and a curvature radius r6 of an imageplane-side surface thereof are both positive, so as to have a shape of ameniscus lens directing a convex surface to the object side near theoptical axis X. The shape of the third lens L3 is not limited to the onein Numerical Data Example 1. The third lens L3 can be formed in anyshape as long as the curvature radius r5 of the object-side surfacethereof is positive. For example, the third lens L3 can also be formedin a shape such that the curvature radius r6 of the image plane-sidesurface thereof is negative, i.e., a shape of a biconvex lens near theoptical axis X.

The second lens group G2 includes a fourth lens L4 having negativerefractive power and a fifth lens L5 having negative refractive power,arranged in the order from the object side. Among them, the fourth lensL4 is formed in a shape such that a curvature radius r7 of anobject-side surface thereof and a curvature radius r8 of an imageplane-side surface thereof are both negative, so as to have a shape of ameniscus lens directing a concave surface to the object side near theoptical axis X.

The fifth lens L5 is formed in a shape such that a curvature radius r9of an object-side surface thereof and a curvature radius r10 of an imageplane-side surface thereof are both positive, so as to have a shape of ameniscus lens directing a convex surface to the object side near theoptical axis X. Here, the shape of the fifth lens L5 is not limited tothe one in Numerical Data Example 1. The fifth lens L5 can also beformed in a shape such that the curvature radius r9 of the object-sidesurface thereof and the curvature radius r10 of the image plane-sidesurface thereof are both negative, i.e., a shape of a meniscus lensdirecting a concave surface to the object side near the optical axis X.Alternatively, the fifth lens L5 can also be formed in a shape such thatthe curvature radius r9 of the object-side surface thereof is negativeand the curvature radius r10 of the image plane-side surface thereof ispositive, i.e., a shape of a biconcave lens near the optical axis X.Numerical Data Example 3 is an example, in which the fifth lens L5 isformed in a shape of a meniscus lens directing a concave surface to theobject side near the optical axis X.

The third lens group G3 includes a sixth lens L6 having positiverefractive power and the seventh lens L7 having negative refractivepower, arranged in the order from the object side. The sixth lens L6 isformed in a shape such that a curvature radius r11 of an object-sidesurface thereof and a curvature radius r12 of an image plane-sidesurface thereof are both positive, so as to have a shape of a meniscuslens directing a convex surface to the object side near the optical axisX. In addition, the seventh lens L7 is formed in a shape such that acurvature radius r13 of an object-side surface thereof and a curvatureradius r14 of an image plane-side surface thereof are both positive, soas to have a shape of a meniscus lens directing a convex surface thereofto the object side near the optical axis X.

In the sixth lens L6 and the seventh lens L7, the object-side surfacesthereof and the image plane-side surfaces thereof are formed as asphericshapes having inflexion points, and are formed in shapes so as to havestrong positive refractive powers toward the lens peripheries from theoptical axis X. With those shapes of the sixth lens L6 and the seventhlens L7, it is possible to satisfactorily correct an off-axis chromaticaberration of magnification as well as an axial chromatic aberration. Inaddition, it is also possible to suitably restrain the incident angle ofa light beam emitted from the imaging lens to the image plane IM withinthe range of a chief ray angle (CRA).

Here, according to the embodiment, both the object-side surfaces and theimage plane-side surfaces of the sixth lens L6 and the seventh lens L7are formed as aspheric shapes having inflexion points. However, it isnot necessary to form the both surfaces as aspheric shapes havinginflexion points. Even when one of those surfaces is formed as anaspheric shape having an inflexion point, it is still possible to formone or both of the sixth lens L6 and the seventh lens L7 in a shape soas to have strong positive refractive power toward the lens peripheryfrom the optical axis X. Moreover, depending on required opticalperformance and/or the degree of downsizing of the imaging lens, it maynot be necessary to provide an inflexion point on the sixth lens L6 andthe seventh lens L7.

The imaging lens of the embodiment satisfies the following conditionalexpressions (1) to (15):40<νd1<75  (1)20<νd2<35  (2)40<νd3<75  (3)40<νd6<75  (4)20<νd7<35  (5)20<νd4<35  (6)20<νd5<35  (7)0.02<D56/f<0.15  (8)0.6<f123/f<1.2  (9)−15<f67/f<−1.5  (10)−2<f45/f6<−0.1  (11)−15<f4/f<−3  (12)0.5<f1/f<2.0  (13)−4<f2/f<−0.5  (14)1<f3/f<4  (15)

In the above conditional expressions:

νd1: Abbe's number of a first lens L1

νd2: Abbe's number of a second lens L2

νd3: Abbe's number of a third lens L3

νd4: Abbe's number of a fourth lens L4

νd5: Abbe's number of a fifth lens L5

νd6: Abbe's number of a sixth lens L6

νd7: Abbe's number of a seventh lens L7

f: Focal length of a whole lens system

f1: Focal length of the first lens L1

f2: Focal length of the second lens L2

f3: Focal length of the third lens L3

f4: Focal length of the fourth lens L4

f6: Focal length of the sixth lens L6

f45: Composite focal length of the fourth lens L4 and the fifth lens L5

f67: Composite focal length of the sixth lens L6 and the seventh lens L7

f123: Composite focal length of the lenses from the first lens L1 to thethird lens L3

D56: Distance on an optical axis X between the fifth lens L5 and thesixth lens L6

In order to more satisfactorily correct aberrations, the imaging lens ofthe embodiment satisfies the following conditional expressions (10A) and(12A):−12<f67/f<−1.5  (10A)−12<f4/f<−3  (12A)

Here, it is not necessary to satisfy all of the above conditionalexpressions, and it is achievable to obtain an effect corresponding tothe respective conditional expressions when any single one of the aboveconditional expressions is individually satisfied.

In the embodiment, all lens surfaces of the respective lenses are formedas an aspheric surface. When the aspheric shapes applied to the lenssurfaces have an axis Z in a direction of the optical axis X, a height Hin a direction perpendicular to the optical axis X, a conic constant k,and aspheric coefficients A₄, A₆, A₈, A₁₀, A₁₂, A₁₄, and A₁₆, the shapesof the aspheric surfaces of the lens surfaces are expressed as follows:

$\begin{matrix}{Z = {\frac{\frac{H^{2}}{R}}{1 + \sqrt{1 - {\left( {k + 1} \right)\frac{H^{2}}{R^{2}}}}} + {A_{4}H^{4}} + {A_{6}H^{6}} + {A_{8}H^{8}} + {A_{10}H^{10}} + {A_{12}H^{12}} + {A_{14}H^{14}} + {A_{16}H^{16}}}} & \left\lbrack {{Formula}\mspace{14mu} 1} \right\rbrack\end{matrix}$

Next, Numerical Data Examples of the imaging lens of the embodiment willbe described. In each Numerical Data Example, f represents a focallength of the whole lens system, Fno represents an F number, and ωrepresents a half angle of view, respectively. In addition, i representsa surface number counted from the object side, r represents a curvatureradius, d represents a distance between lens surfaces (surface spacing)on the optical axis, nd represents a refractive index, and νd representsan Abbe's number, respectively. Here, aspheric surfaces are indicatedwith surface numbers i affixed with * (asterisk).

Numerical Data Example 1

Basic lens data are shown below. f = 8.04 mm, Fno = 1.8, ω = 36.7° Unit:mm Surface Data Surface Number i r d nd νd (Object) ∞ ∞  1* 3.533 1.3151.5346 56.1 (=νd1)  2* (Stop) 32.140 0.067  3* 9.059 0.365 1.6355 24.0(=νd2)  4* 4.420 0.076  5* 5.948 0.701 1.5346 56.1 (=νd3)  6* 18.2261.016  7* −3.745 0.330 1.6355 24.0 (=νd4)  8* −4.940 0.101  9* 30.2171.053 1.6355 24.0 (=νd5) 10* 20.289 0.394 (=D56) 11* 4.406 1.095 1.534656.1 (=νd6) 12* 5.672 0.698 13* 7.325 1.425 1.6355 24.0 (=νd7) 14* 3.7530.440 15 ∞ 0.300 1.5168 64.2 16 ∞ 0.530 (Image ∞ plane) Aspheric SurfaceData First Surface k = 0.000, A₄ = −1.830E−03, A₆ = 1.363E−04, A₈ =−1.227E−04, A₁₀ = 2.595E−07, A₁₂ = −2.790E−07, A₁₄ = −8.280E−08, A₁₆ =8.141E−09 Second Surface k = 0.000, A₄ = 1.280E−02, A₆ = −1.457E−02, A₈= 5.183E−03, A₁₀ = −9.113E−04, A₁₂ = 5.259E−05, A₁₄ = 5.804E−06, A₁₆ =−7.418E−07 Third Surface k = 0.000, A₄ = 1.459E−02, A₆ = −2.057E−02, A₈= 7.412E−03, A₁₀ = −1.296E−03, A₁₂ = 9.735E−05, A₁₄ = 1.620E−06, A₁₆ =−5.796E−07 Fourth Surface k = 0.000, A₄ = 5.572E−03, A₆ = −1.275E−02, A₈= 3.429E−03, A₁₀ = −3.506E−04, A₁₂ = 1.621E−06, A₁₄ = −4.572E−07, A₁₆ =1.498E−07 Fifth Surface k = 0.000, A₄ = 5.066E−03, A₆ = −3.926E−03, A₈ =1.347E−03, A₁₀ = −1.231E−04, A₁₂ = −2.627E−07, A₁₄ = 9.933E−07, A₁₆ =−4.663E−08 Sixth Surface k = 0.000, A₄ = −3.072E−03, A₆ = 7.384E−04, A₈= 9.673E−04, A₁₀ = −3.384E−04, A₁₂ = 2.739E−05, A₁₄ = 5.139E−06, A₁₆ =−9.157E−07 Seventh Surface k = 0.000, A₄ = −1.163E−02, A₆ = 1.853E−03,A₈ = −8.807E−07, A₁₀ = −2.749E−05, A₁₂ = −1.385E−05, A₁₄ = 1.477E−06,A₁₆ = 3.064E−07 Eighth Surface k = 0.000, A₄ = −1.143E−02, A₆ =2.318E−03, A₈ = 5.775E−06, A₁₀ = 7.657E−06, A₁₂ = −8.628E−07, A₁₄ =−1.810E−06, A₁₆ = 6.733E−07 Ninth Surface k = 0.000, A₄ = −5.674E−03, A₆= −6.296E−04, A₈ = 4.171E−05, A₁₀ = −8.677E−06, A₁₂ = −3.752E−07, A₁₄ =8.901E−08, A₁₆ = −2.474E−08 Tenth Surface k = 0.000, A₄ = −6.851E−03, A₆= −1.387E−04, A₈ = 5.738E−05, A₁₀ = −3.989E−06, A₁₂ = 2.015E−07, A₁₄ =−1.889E−09, A₁₆ = −1.030E−09 Eleventh Surface k = 0.000, A₄ =−1.075E−02, A₆ = −1.820E−05, A₈ = 2.366E−06, A₁₀ = 5.268E−07, A₁₂ =−4.773E−09, A₁₄ = 4.042E−10, A₁₆ = −9.365E−11 Twelfth Surface k = 0.000,A₄ = −5.711E−03, A₆ = −3.528E−04, A₈ = 3.504E−05, A₁₀ = −1.708E−06, A₁₂= 3.413E−08, A₁₄ = 1.354E−10, A₁₆ = −1.309E−11 Thirteenth Surface k =0.000, A₄ = −2.086E−02, A₆ = 1.367E−03, A₈ = −3.316E−05, A₁₀ =−2.029E−08, A₁₂ = 5.364E−09, A₁₄ = 2.437E−11, A₁₆ = 2.910E−12 FourteenthSurface k = −6.723, A₄ = −8.556E−03, A₆ = 4.592E−04, A₈ = −1.667E−05,A₁₀ = 2.942E−07, A₁₂ = 1.150E−08, A₁₄ = −6.750E−10, A₁₆ = 8.820E−12 f1 =7.31 mm f2 = −14.01 mm f3 = 16.19 mm f4 = −27.27 mm f5 = −101.34 mm f6 =28.38 mm f7 = −14.33 mm f45 = −20.98 mm f67 = −46.34 mm f123 = 7.64 mmThe values of the respective conditional expressions are as follows:D56/f = 0.05 f1/f = 0.91 f2/f = −1.74 f3/f = 2.02 f4/f = −3.39 f67/f =−5.77 f45/f6 = −0.74 f123/f = 0.95

Accordingly, the imaging lens of Numerical Data Example 1 satisfies theabove-described conditional expressions. The distance on the opticalaxis X from the object-side surface of the first lens L1 to the imageplane IM (length in air for the filter 10) is 9.80 mm, and downsizing ofthe imaging lens is attained.

FIG. 2 shows a lateral aberration that corresponds to a ratio H of eachimage height to the maximum image height (hereinafter referred to as“image height ratio H”) in the imaging lens of Numerical Data Example 1,which is divided into a tangential direction and a sagittal direction(The same is true for FIGS. 5, 8, 11, 14, and 17). Furthermore, FIG. 3shows a spherical aberration (mm), astigmatism (mm), and a distortion(%), respectively, of the imaging lens of Numerical Data Example 1. Inthe aberration diagrams, for the lateral aberration diagrams andspherical aberration diagrams, aberrations at respective wavelengths,i.e. a g line (435.84 nm), an e line (546.07 nm), and a C line (656.27nm) are indicated. In the astigmatism diagram, an aberration on asagittal image surface S and an aberration on a tangential image surfaceT are respectively indicated (The same is true for FIGS. 6, 9, 12, 15,and 18). As shown in FIGS. 2 and 3, according to the imaging lens ofNumerical Data Example 1, the aberrations are satisfactorily corrected.

Numerical Data Example 2

Basic lens data are shown below. f = 7.94 mm, Fno = 1.8, ω = 37.1° Unit:mm Surface Data Surface Number i r d nd νd (Object) ∞ ∞  1* 3.557 1.2351.5346 56.1 (=νd1)  2* (Stop) 32.077 0.080  3* 9.575 0.371 1.6355 24.0(=νd2)  4* 4.489 0.077  5* 6.066 0.648 1.5346 56.1 (=νd3)  6* 17.5170.976  7* −3.765 0.507 1.6355 24.0 (=νd4)  8* −4.237 0.047  9* 33.8930.818 1.6355 24.0 (=νd5) 10* 22.281 1.062 (=D56) 11* 4.498 1.090 1.534656.1 (=νd6) 12* 5.358 0.679 13* 6.805 1.030 1.6355 24.0 (=νd7) 14* 3.6800.440 15 ∞ 0.300 1.5168 64.2 16 ∞ 0.530 (Image ∞ plane) Aspheric SurfaceData First Surface k = 0.000, A₄ = −1.726E−03, A₆ = 1.683E−04, A₈ =−1.209E−04, A₁₀ = −4.321E−08, A₁₂ = −4.405E−07, A₁₄ = −1.069E−07, A₁₆ =8.333E−09 Second Surface k = 0.000, A₄ = 1.292E−02, A₆ = −1.457E−02, A₈= 5.182E−03, A₁₀ = −9.118E−04, A₁₂ = 5.248E−05, A₁₄ = 5.791E−06, A₁₆ =−7.380E−07 Third Surface k = 0.000, A₄ = 1.456E−02, A₆ = −2.055E−02, A₈= 7.420E−03, A₁₀ = −1.295E−03, A₁₂ = 9.758E−05, A₁₄ = 1.604E−06, A₁₆ =−6.025E−07 Fourth Surface k = 0.000, A₄ = 5.582E−03, A₆ = −1.276E−02, A₈= 3.429E−03, A₁₀ = −3.507E−04, A₁₂ = 1.532E−06, A₁₄ = −4.954E−07, A₁₆ =1.375E−07 Fifth Surface k = 0.000, A₄ = 4.583E−03, A₆ = −3.932E−03, A₈ =1.338E−03, A₁₀ = −1.251E−04, A₁₂ = −5.200E−07, A₁₄ = 9.596E−07, A₁₆ =−4.592E−08 Sixth Surface k = 0.000, A₄ = −3.136E−03, A₆ = 7.503E−04, A₈= 9.754E−04, A₁₀ = −3.388E−04, A₁₂ = 2.684E−05, A₁₄ = 4.994E−06, A₁₆ =−9.459E−07 Seventh Surface k = 0.000, A₄ = −1.232E−02, A₆ = 1.820E−03,A₈ = 3.482E−06, A₁₀ =−2.652E−05, A₁₂ = −1.373E−05, A₁₄ = 1.425E−06, A₁₆= 2.744E−07 Eighth Surface k = 0.000, A₄ = −1.064E−02, A₆ = 2.321E−03,A₈ = −3.718E−06, A₁₀ = 5.205E−06, A₁₂ = −1.569E−06, A₁₄ = −1.971E−06,A₁₆ = 6.443E−07 Ninth Surface k = 0.000, A₄ = −8.793E−03, A₆ =−6.347E−04, A₈ = 8.162E−05, A₁₀ = −7.303E−06, A₁₂ = −6.511E−07, A₁₄ =1.035E−08, A₁₆ = −4.041E−08 Tenth Surface k = 0.000, A₄ = −9.201E−03, A₆= −2.143E−05, A₈ = 5.445E−05, A₁₀ = −4.648E−06, A₁₂ = 1.527E−07, A₁₄ =−5.252E−09, A₁₆ = −1.420E−09 Eleventh Surface k = 0.000, A₄ =−9.386E−03, A₆ = −3.833E−05, A₈ = −1.706E−06, A₁₀ = 4.515E−07, A₁₂ =−2.894E−09, A₁₄ = 6.350E−10, A₁₆ = −7.863E−11 Twelfth Surface k = 0.000,A₄ = −5.857E−03, A₆ = −3.841E−04, A₈ = 3.712E−05, A₁₀ = −1.617E−06, A₁₂= 3.448E−08, A₁₄ = 1.940E−11, A₁₆ = −2.053E−11 Thirteenth Surface k =0.000, A₄ = −2.058E−02, A₆ = 1.357E−03, A₈ = −3.344E−05, A₁₀ =−2.400E−08, A₁₂ = 5.287E−09, A₁₄ = 2.116E−11, A₁₆ = 2.673E−12 FourteenthSurface k = −7.024, A₄ = −7.543E−03, A₆ = 4.526E−04, A₈ = −1.720E−05,A₁₀ = 2.880E−07, A₁₂ = 1.156E−08, A₁₄ = −6.712E−10, A₁₆ = 8.883E−12 f1 =7.37 mm f2 = −13.69 mm f3 = 17.02 mm f4 = −91.33 mm f5 = −105.21 mm f6 =36.38 mm f7 = −14.46 mm f45 = −47.36 mm f67 = −31.69 mm f123 = 7.96 mmThe values of the respective conditional expressions are as follows:D56/f = 0.13 f1/f = 0.93 f2/f = −1.72 f3/f = 2.14 f4/f = −11.50 f67/f =−3.99 f45/f6 = −1.30 f123/f = 1.00

Accordingly, the imaging lens of Numerical Data Example 2 satisfies theabove-described conditional expressions. The distance on the opticalaxis X from the object-side surface of the first lens L1 to the imageplane IM (length in air for the filter 10) is 9.79 mm, and downsizing ofthe imaging lens is attained.

FIG. 5 shows a lateral aberration that corresponds to the image heightratio H, and FIG. 6 shows a spherical aberration (mm), astigmatism (mm),and a distortion (%), respectively, of the imaging lens of NumericalData Example 2. As shown in FIGS. 5 and 6, according to the imaging lensof Numerical Data Example 2, the aberrations are also satisfactorilycorrected.

Numerical Data Example 3

Basic lens data are shown below. f = 10.88 mm, Fno = 2.1, ω = 28.9°Unit: mm Surface Data Surface Number i r d nd νd (Object) ∞ ∞  1* 3.3002.430 1.5346 56.1 (=νd1)  2* (Stop) −311.769 0.049  3* 15.636 0.2961.6355 24.0 (=νd2)  4* 4.847 0.134  5* 8.086 0.541 1.5346 56.1 (=νd3) 6* 17.887 1.152  7* −3.268 0.492 1.6355 24.0 (=νd4)  8* −3.911 0.050 9* −10.323 2.024 1.6355 24.0 (=νd5) 10* −17.420 0.409 (=D56) 11* 8.9270.646 1.5346 56.1 (=νd6) 12* 10.432 0.700 13* 13.148 0.760 1.6355 24.0(=νd7) 14* 5.511 0.440 15 ∞ 0.300 1.5168 64.2 16 ∞ 1.131 (Image ∞ plane)Aspheric Surface Data First Surface k = 0.000, A₄ = −1.038E−03, A₆ =3.430E−04, A₈ = −8.024E−05, A₁₀ = 6.292E−06, A₁₂ = 2.127E−07, A₁₄ =−5.376E−08, A₁₆ = −5.718E−10 Second Surface k = 0.000, A₄ = 1.842E−02,A₆ = −1.448E−02, A₈ = 5.161E−03, A₁₀ = −9.132E−04, A₁₂ = 5.236E−05, A₁₄= 5.824E−06, A₁₆ = −7.112E−07 Third Surface k = 0.000, A₄ = 1.704E−02,A₆ = −2.025E−02, A₈ = 7.416E−03, A₁₀ = −1.305E−03, A₁₂ = 9.570E−05, A₁₄= 1.656E−06, A₁₆ = −4.532E−07 Fourth Surface k = 0.000, A₄ = 6.821E−03,A₆ = −1.205E−02, A₈ = 3.471E−03, A₁₀ = −3.456E−04, A₁₂ = 3.834E−06, A₁₄= 1.155E−07, A₁₆ = 2.306E−07 Fifth Surface k = 0.000, A₄ = 4.042E−03, A₆= −4.732E−03, A₈ = 1.319E−03, A₁₀ = −1.148E−04, A₁₂ = 1.088E−06, A₁₄ =1.034E−06, A₁₆ = −3.437E−08 Sixth Surface k = 0.000, A₄ = −4.938E−03, A₆= 1.613E−04, A₈ = 9.595E−04, A₁₀ = −3.361E−04, A₁₂ = 2.670E−05, A₁₄ =4.836E−06, A₁₆ = −1.031E−06 Seventh Surface k = 0.000, A₄ = −8.177E−03,A₆ = 1.125E−03, A₈ = −9.875E−05, A₁₀ = −4.778E−05, A₁₂ = −1.854E−05, A₁₄= 1.300E−06, A₁₆ = 4.278E−07 Eighth Surface k = 0.000, A₄ = −8.574E−03,A₆ = 1.865E−03, A₈ = −1.597E−04, A₁₀ = −1.638E−05, A₁₂ = −3.099E−06, A₁₄= −1.833E−06, A₁₆ = 7.218E−07 Ninth Surface k = 0.000, A₄ = −7.660E−03,A₆ = −5.036E−04, A₈ = −4.274E−06, A₁₀ = −2.335E−05, A₁₂ = −1.854E−06,A₁₄ = 2.960E−07, A₁₆ = 3.958E−08 Tenth Surface k = 0.000, A₄ =−4.613E−03, A₆ = −1.808E−04, A₈ = 6.170E−05, A₁₀ = −3.871E−06, A₁₂ =1.859E−07, A₁₄ = −1.096E−09, A₁₆ = −4.257E−10 Eleventh Surface k =0.000, A₄ = −1.110E−02, A₆ = 4.474E−05, A₈ = 9.432E−06, A₁₀ = 7.902E−07,A₁₂ = 1.870E−09, A₁₄ = 3.984E−10, A₁₆ = −1.193E−10 Twelfth Surface k =0.000, A₄ = −7.493E−03, A₆ = −2.431E−04, A₈ = 3.817E−05, A₁₀ =−1.743E−06, A₁₂ = 3.133E−08, A₁₄ = 2.160E−10, A₁₆ = 5.987E−12 ThirteenthSurface k = 0.000, A₄ = −1.939E−02, A₆ = 1.379E−03, A₈ = −3.268E−05, A₁₀= −5.612E−09, A₁₂ = 5.547E−09, A₁₄ = 7.726E−12, A₁₆ = 1.206E−12Fourteenth Surface k = −1.661E+01, A₄ = −1.191E−02, A₆ = 6.454E−04, A₈ =−1.707E−05, A₁₀ = 2.452E−07, A₁₂ = 1.012E−08, A₁₄ = −6.891E−10, A₁₆ =1.006E−11 f1 = 6.12 mm f2 = −11.17 mm f3 = 27.08 mm f4 = −44.47 mm f5 =−44.83 mm f6 = 100.70 mm f7 = −15.53 mm f45 = −22.17 mm f67 = −19.29 mmf123 = 7.83 mm The values of the respective conditional expressions areas follows: D56/f = 0.04 f1/f = 0.56 f2/f = −1.03 f3/f = 2.49 f4/f =−4.09 f67/f = −1.77 f45/f6 = −0.22 f123/f = 0.72

Accordingly, the imaging lens of Numerical Data Example 3 satisfies theabove-described conditional expressions. The distance on the opticalaxis X from the object-side surface of the first lens L1 to the imageplane IM (length in air for the filter 10) is 11.45 mm, and downsizingof the imaging lens is attained.

FIG. 8 shows a lateral aberration that corresponds to the image heightratio H and FIG. 9 shows a spherical aberration (mm), astigmatism (mm),and a distortion (%), respectively, of the imaging lens of NumericalData Example 3. As shown in FIGS. 8 and 9, according to the imaging lensof Numerical Data Example 3, the aberrations are also satisfactorilycorrected.

Numerical Data Example 4

Basic lens data are shown below. f = 7.60 mm, Fno = 1.8, ω = 38.3° Unit:mm Surface Data Surface Number i r d nd νd (Object) ∞ ∞  1* 3.529 1.3171.5346 56.1 (=νd1)  2* (Stop) 33.438 0.049  3* 7.726 0.342 1.6355 24.0(=νd2)  4* 4.706 0.102  5* 7.886 0.619 1.5346 56.1 (=νd3)  6* 34.5160.927  7* −3.697 0.503 1.6355 24.0 (=νd4)  8* −4.776 0.050  9* 48.9821.083 1.6355 24.0 (=νd5) 10* 24.422 0.297 (=D56) 11* 4.582 1.054 1.534656.1 (=νd6) 12* 5.774 0.608 13* 7.279 1.416 1.6355 24.0 (=νd7) 14* 3.6970.440 15 ∞ 0.300 1.5168 64.2 16 ∞ 0.530 (Image ∞ plane) Aspheric SurfaceData First Surface k = 0.000, A₄ = −2.152E−03, A₆ = 1.571E−04, A₈ =−1.329E−04, A₁₀ = −2.775E−06, A₁₂ = −6.955E−07, A₁₄ = −9.756E−08, A₁₆ =2.094E−08 Second Surface k = 0.000, A₄ = 1.297E−02, A₆ = −1.458E−02, A₈= 5.172E−03, A₁₀ = −9.133E−04, A₁₂ = 5.234E−05, A₁₄ = 5.794E−06, A₁₆ =−7.303E−07 Third Surface k = 0.000, A₄ = 1.428E−02, A₆ = −2.060E−02, A₈= 7.409E−03, A₁₀ = −1.297E−03, A₁₂ = 9.705E−05, A₁₄ = 1.548E−06, A₁₆ =−5.924E−07 Fourth Surface k = 0.000, A₄ = 5.601E−03, A₆ = −1.275E−02, A₈= 3.424E−03, A₁₀ = −3.521E−04, A₁₂ = 1.209E−06, A₁₄ = −5.725E−07, A₁₆ =1.186E−07 Fifth Surface k = 0.000, A₄ = 6.052E−03, A₆ = −3.836E−03, A₈ =1.352E−03, A₁₀ = −1.240E−04, A₁₂ = −5.950E−07, A₁₄ = 9.220E−07, A₁₆ =−5.702E−08 Sixth Surface k = 0.000, A₄ = −3.130E−03, A₆ = 6.224E−04, A₈= 9.555E−04, A₁₀ = −3.405E−04, A₁₂ = 2.696E−05, A₁₄ = 5.073E−06, A₁₆ =−9.220E−07 Seventh Surface k = 0.000, A₄ = −1.157E−02, A₆ = 1.845E−03,A₈ = −2.713E−06, A₁₀ = −2.778E−05, A₁₂ = −1.401E−05, A₁₄ = 1.382E−06,A₁₆ = 2.677E−07 Eighth Surface k = 0.000, A₄ = −1.124E−02, A₆ =2.411E−03, A₈ = 9.544E−06, A₁₀ = 5.236E−06, A₁₂ = −1.552E−06, A₁₄ =−1.909E−06, A₁₆ = 6.714E−07 Ninth Surface k = 0.000, A₄ = −4.523E−03, A₆= −5.470E−04, A₈ = 2.810E−05, A₁₀ = −1.175E−05, A₁₂ = −7.069E−07, A₁₄ =8.915E−08, A₁₆ = −1.659E−08 Tenth Surface k = 0.000, A₄ = −5.602E−03, A₆= −1.464E−04, A₈ = 5.674E−05, A₁₀ = −4.007E−06, A₁₂ = 2.015E−07, A₁₄ =−1.075E−09, A₁₆ = −8.115E−10 Eleventh Surface k = 0.000, A₄ =−1.161E−02, A₆ = 3.886E−05, A₈ = 3.992E−06, A₁₀ = 5.577E−07, A₁₂ =−4.023E−09, A₁₄ = 4.113E−10, A₁₆ = −9.561E−10 Twelfth Surface k = 0.000,A₄ = −5.729E−03, A₆ = −3.820E−04, A₈ = 3.626E−05, A₁₀ = −1.640E−06, A₁₂= 3.512E−08, A₁₄ = 8.914E−11, A₁₆ = −1.691E−11 Thirteenth Surface k =0.000, A₄ = −2.061E−02, A₆ = 1.380E−03, A₈ = −3.293E−05, A₁₀ =−1.823E−08, A₁₂ = 5.235E−09, A₁₄ = 1.298E−11, A₁₆ = 2.274E−12 FourteenthSurface k = −7.048, A₄ = −8.102E−03, A₆ = 4.452E−04, A₈ = −1.654E−05,A₁₀ = 3.003E−07, A₁₂ = 1.157E−08, A₁₄ = −6.759E−10, A₁₆ = 8.719E−12 f1 =7.27 mm f2 = −19.82 mm f3 = 18.97 mm f4 = −31.48 mm f5 = −77.98 mm f6 =31.74 mm f7 = −13.97 mm f45 = −21.82 mm f67 = −35.34 mm f123 = 7.08 mmThe values of the respective conditional expressions are as follows:D56/f = 0.04 f1/f = 0.96 f2/f = −2.61 f3/f = 2.50 f4/f = −4.14 f67/f =−4.65 f45/f6 = −0.69 f123/f = 0.93

Accordingly, the imaging lens of Numerical Data Example 4 satisfies theabove-described conditional expressions. The distance on the opticalaxis X from the object-side surface of the first lens L1 to the imageplane IM (length in air for the filter 10) is 9.53 mm, and downsizing ofthe imaging lens is attained.

FIG. 11 shows a lateral aberration that corresponds to the image heightratio H and FIG. 12 shows a spherical aberration (mm), astigmatism (mm),and a distortion (%), respectively, of the imaging lens of NumericalData Example 4. As shown in FIGS. 11 and 12, according to the imaginglens of Numerical Data Example 4, the aberrations are alsosatisfactorily corrected.

Numerical Data Example 5

Basic lens data are shown below. f = 8.23 mm, Fno = 2.0, ω = 36.1° Unit:mm Surface Data Surface Number i r d nd νd (Object) ∞ ∞  1* 4.001 1.3631.5346 56.1 (=νd1)  2* (Stop) 35.292 0.152  3* 13.633 0.509 1.6355 24.0(=νd2)  4* 3.623 0.056  5* 3.901 0.750 1.5346 56.1 (=νd3)  6* 20.4601.063  7* −3.905 0.285 1.6355 24.0 (=νd4)  8* −4.397 0.083  9* 21.5311.014 1.6355 24.0 (=νd5) 10* 15.822 0.319 (=D56) 11* 4.348 1.181 1.534656.1 (=νd6) 12* 5.641 0.781 13* 6.246 1.537 1.6355 24.0 (=νd7) 14* 3.4810.440 15 ∞ 0.300 1.5168 64.2 16 ∞ 0.710 (Image ∞ plane) Aspheric SurfaceData First Surface k = 0.000, A₄ = −1.574E−03, A₆ = 5.572E−05, A₈ =−1.146E−04, A₁₀ = 4.563E−06, A₁₂ = 4.723E−07, A₁₄ = −5.047E−08, A₁₆ =−1.997E−08 Second Surface k = 0.000, A₄ = 1.329E−02, A₆ = −1.471E−02, A₈= 5.143E−03, A₁₀ = −9.126E−04, A₁₂ = 5.367E−05, A₁₄ = 6.015E−06, A₁₆ =−8.135E−07 Third Surface k = 0.000, A₄ = 1.603E−02, A₆ = −2.040E−02, A₈= 7.418E−03, A₁₀ = −1.305E−03, A₁₂ = 9.477E−05, A₁₄ = 1.430E−06, A₁₆ =−4.258E−07 Fourth Surface k = 0.000, A₄ = 4.026E−03, A₆ = −1.280E−02, A₈= 3.416E−03, A₁₀ = −3.539E−04, A₁₂ = 1.335E−06, A₁₄ = −3.641E−07, A₁₆ =2.086E−07 Fifth Surface k = 0.000, A₄ = 1.803E−03, A₆ = −4.300E−03, A₈ =1.320E−03, A₁₀ = −1.243E−04, A₁₂ = −1.962E−07, A₁₄ = 1.021E−06, A₁₆ =−3.326E−08 Sixth Surface k = 0.000, A₄ = −2.484E−03, A₆ = 1.224E−03, A₈= 9.914E−04, A₁₀ = −3.372E−04, A₁₂ = 2.765E−05, A₁₄ = 5.270E−06, A₁₆ =−8.886E−07 Seventh Surface k = 0.000, A₄ = −1.188E−02, A₆ = 1.765E−03,A₈ = 1.543E−05, A₁₀ = −2.385E−05, A₁₂ = −1.347E−05, A₁₄ = 1.447E−06, A₁₆= 2.900E−07 Eighth Surface k = 0.000, A₄ = −1.309E−02, A₆ = 2.037E−03,A₈ = −4.695E−05, A₁₀ = −5.699E−07, A₁₂ = −2.191E−06, A₁₄ = −2.017E−06,A₁₆ = 6.334E−07 Ninth Surface k = 0.000, A₄ = −5.313E−03, A₆ =−5.971E−04, A₈ = 5.060E−05, A₁₀ = −8.367E−06, A₁₂ = −2.573E−07, A₁₄ =1.203E−07, A₁₆ = −1.622E−08 Tenth Surface k = 0.000, A₄ = −8.340E−03, A₆= −1.896E−04, A₈ = 5.416E−05, A₁₀ = −4.072E−06, A₁₂ = 2.098E−07, A₁₄ =−2.675E−10, A₁₆ = −8.739E−10 Eleventh Surface k = 0.000, A₄ =−1.125E−02, A₆ = −2.212E−05, A₈ = 2.165E−06, A₁₀ = 5.092E−07, A₁₂ =−5.409E−09, A₁₄ = 4.063E−10, A₁₆ = −9.054E−11 Twelfth Surface k = 0.000,A₄ = −5.146E−03, A₆ = −3.399E−04, A₈ = 3.516E−05, A₁₀ = −1.702E−06, A₁₂= 3.409E−08, A₁₄ = 1.156E−10, A₁₆ = −1.440E−11 Thirteenth Surface k =0.000, A₄ = −2.129E−02, A₆ = 1.361E−03, A₈ = −3.313E−05, A₁₀ =−1.711E−08, A₁₂ = 5.519E−09, A₁₄ = 2.890E−11, A₁₆ = 3.019E−12 FourteenthSurface k = −5.675, A₄ = −8.164E−03, A₆ = 4.582E−04, A₈ = −1.680E−05,A₁₀ = 2.931E−07, A₁₂ = 1.156E−08, A₁₄ = −6.697E−10, A₁₆ = 9.002E−12 f1 =8.32 mm f2 = −7.92 mm f3 = 8.88 mm f4 = −70.85 mm f5 = −100.86 mm f6 =26.92 mm f7 = −15.78 mm f45 = −40.53 mm f67 = −83.33 mm f123 = 9.12 mmThe values of the respective conditional expressions are as follows:D56/f = 0.04 f1/f = 1.01 f2/f = −0.96 f3/f = 1.08 f4/f = −8.61 f67/f =−10.13 f45/f6 = −1.51 f123/f = 1.11

Accordingly, the imaging lens of Numerical Data Example 5 satisfies theabove-described conditional expressions. The distance on the opticalaxis X from the object-side surface of the first lens L1 to the imageplane IM (length in air for the filter 10) is 10.44 mm, and downsizingof the imaging lens is attained.

FIG. 14 shows a lateral aberration that corresponds to the image heightratio H and FIG. 15 shows a spherical aberration (mm), astigmatism (mm),and a distortion (%), respectively, of the imaging lens of NumericalData Example 5. As shown in FIGS. 14 and 15, according to the imaginglens of Numerical Data Example 5, the aberrations are alsosatisfactorily corrected.

Numerical Data Example 6

Basic lens data are shown below. f = 7.13 mm, Fno = 1.8, ω = 40.1° Unit:mm Surface Data Surface Number i r d nd νd (Object) ∞ ∞  1* 3.597 1.2241.5346 56.1 (=νd1)  2* (Stop) 35.317 0.065  3* 9.798 0.314 1.6355 24.0(=νd2)  4* 4.606 0.079  5* 6.480 0.608 1.5346 56.1 (=νd3)  6* 26.3880.932  7* −3.825 0.433 1.6355 24.0 (=νd4)  8* −4.241 0.050  9* 31.2620.996 1.6355 24.0 (=νd5) 10* 19.771 0.345 (=D56) 11* 4.466 1.042 1.534656.1 (=νd6) 12* 5.654 0.641 13* 6.499 1.465 1.6355 24.0 (=νd7) 14* 3.7060.440 15 ∞ 0.300 1.5168 64.2 16 ∞ 0.530 (Image ∞ plane) Aspheric SurfaceData First Surface k = 0.000, A₄ = −2.522E−03, A₆ = 1.099E−04, A₈ =−1.485E−04, A₁₀ = −2.443E−06, A₁₂ = −4.628E−07, A₁₄ = −5.002E−08, A₁₆ =6.290E−09 Second Surface k = 0.000, A₄ = 1.270E−02, A₆ = −1.462E−02, A₈= 5.167E−03, A₁₀ = −9.139E−04, A₁₂ = 5.237E−05, A₁₄ = 5.812E−06, A₁₆ =−7.369E−07 Third Surface k = 0.000, A₄ = 1.492E−02, A₆ = −2.053E−02, A₈= 7.421E−03, A₁₀ = −1.297E−03, A₁₂ = 9.670E−05, A₁₄ = 1.396E−06, A₁₆ =−6.286E−07 Fourth Surface k = 0.000, A₄ = 5.576E−03, A₆ = −1.267E−02, A₈= 3.430E−03, A₁₀ = −3.536E−04, A₁₂ = 6.974E−07, A₁₄ = −6.692E−07, A₁₆ =1.037E−07 Fifth Surface k = 0.000, A₄ = 5.354E−03, A₆ = −3.869E−03, A₈ =1.361E−03, A₁₀ = −1.203E−04, A₁₂ = −9.243E−08, A₁₄ = 9.064E−07, A₁₆ =−8.594E−08 Sixth Surface k = 0.000, A₄ = −2.753E−03, A₆ = 7.228E−04, A₈= 9.740E−04, A₁₀ = −3.408E−04, A₁₂ = 2.629E−05, A₁₄ = 4.900E−06, A₁₆ =−9.518E−07 Seventh Surface k = 0.000, A₄ = −1.254E−02, A₆ = 1.885E−03,A₈ = 1.201E−05, A₁₀ = −2.526E−05, A₁₂ = −1.356E−05, A₁₄ = 1.460E−06, A₁₆= 2.920E−07 Eighth Surface k = 0.000, A₄ = −1.071E−02, A₆ = 2.269E−03,A₈ = 9.876E−06, A₁₀ = 8.800E−06, A₁₂ = −5.499E−07, A₁₄ = −1.706E−06, A₁₆= 7.008E−07 Ninth Surface k = 0.000, A₄ = −4.373E−03, A₆ = −4.920E−04,A₈ = 2.796E−05, A₁₀ = −7.886E−06, A₁₂ = −4.923E−08, A₁₄ = 1.211E−07, A₁₆= −2.476E−08 Tenth Surface k = 0.000, A₄ = −7.245E−03, A₆ = −1.221E−04,A₈ = 6.054E−05, A₁₀ = −3.833E−06, A₁₂ = 2.039E−07, A₁₄ = −2.213E−09, A₁₆= −1.144E−09 Eleventh Surface k = 0.000, A₄ = −1.069E−02, A₆ =−2.733E−06, A₈ = 2.429E−06, A₁₀ = 5.305E−07, A₁₂ = −4.447E−09, A₁₄ =4.514E−10, A₁₆ = −8.823E−11 Twelfth Surface k = 0.000, A₄ = −5.109E−03,A₆ = −3.704E−04, A₈ = 3.505E−05, A₁₀ = −1.697E−06, A₁₂ = 3.443E−08, A₁₄= 1.225E−10, A₁₆ = −1.460E−11 Thirteenth Surface k = 0.000, A₄ =−2.099E−02, A₆ = 1.372E−03, A₈ = −3.298E−05, A₁₀ = −1.749E−08, A₁₂ =5.423E−09, A₁₄ = 1.878E−11, A₁₆ = 2.471E−12 Fourteenth Surface k =−5.732, A₄ = −8.088E−03, A₆ = 4.530E−04, A₈ = −1.670E−05, A₁₀ =3.003E−07, A₁₂ = 1.169E−08, A₁₄ = −6.728E−10, A₁₆ = 8.694E−12 f1 = 7.39mm f2 = −14.01 mm f3 = 15.90 mm f4 = −102.92 mm f5 = −87.59 mm f6 =30.44 mm f7 = −17.04 mm f45 = −45.81 mm f67 = −67.65 mm f123 = 7.73 mmThe values of the respective conditional expressions are as follows:D56/f = 0.05 f1/f = 1.04 f2/f = −1.96 f3/f = 2.23 f4/f = −14.43 f67/f =−9.48 f45/f6 = −1.51 f123/f = 1.08

Accordingly, the imaging lens of Numerical Data Example 6 satisfies theabove-described conditional expressions. The distance on the opticalaxis X from the object-side surface of the first lens L1 to the imageplane IM (length in air for the filter 10) is 9.36 mm, and downsizing ofthe imaging lens is attained.

FIG. 17 shows a lateral aberration that corresponds to the image heightratio H and FIG. 18 shows a spherical aberration (mm), astigmatism (mm),and a distortion (%), respectively, of the imaging lens of NumericalData Example 6. As shown in FIGS. 17 and 18, according to the imaginglens of Numerical Data Example 6, the aberrations are alsosatisfactorily corrected.

According to the imaging lens of the embodiment described above, it isachievable to have an angle of view (2ω) that is as wide as 80° orlarger. Here, the imaging lenses of the above-described Numerical DataExamples 1 through 6 have angles of view that are as wide as 57.8° to80.2°. According to the imaging lens of the embodiment, it is possibleto take an image over a wider range than that taken by a conventionalimaging lens.

Furthermore, in these years, with advancement in digital zoom technologyfor enlarging any area of an image obtained through an imaging lens byimage processing, it becomes more common to use an imaging elementhaving a high pixel count in combination with a high-resolution imaginglens. In case of such a high-pixel count imaging element, alight-receiving area of each pixel is smaller, so that an image takentends to be dark. As a method to correct this issue, there is a methodof improving light-receiving sensitivity of the imaging element using anelectrical circuit. However, when the light-receiving sensitivity isincreased, a noise component that does not directly contribute to imageformation is also amplified, so that it is necessary to use anothercircuit to reduce the noise. According to the imaging lenses ofNumerical Data Examples 1 to 6, Fno is very small, as small as 1.8 to2.1. According to the imaging lens of the embodiment, it is possible toobtain sufficiently bright images without providing the above-describedelectrical circuit.

Accordingly, when the imaging lens of the embodiment is applied to animaging optical system such as a camera for mounting in a portabledevice including cellular phones, portable information terminals, andsmartphones, digital still cameras, security cameras, onboard cameras,and network cameras, it is possible to attain both high performance anddownsizing of the cameras.

The present invention is applicable to an imaging lens for mounting in arelatively small-sized camera such as a camera for mounting in aportable device including cellular phones, smartphones, and portableinformation terminals, digital still cameras, security cameras, onboardcameras, and network cameras.

The disclosure of Japanese Patent Application No. 2014-002858, filed onJan. 10, 2014, is incorporated in the application by reference.

While the present invention has been explained with reference to thespecific embodiment of the present invention, the explanation isillustrative and the present invention is limited only by the appendedclaims.

What is claimed is:
 1. An imaging lens comprising: a first lens grouphaving positive refractive power; a second lens group having negativerefractive power; and a third lens group having negative refractivepower, arranged in this order from an object side to an image planeside, wherein said first lens group includes a first lens havingpositive refractive power, a second lens having negative refractivepower, and a third lens having positive refractive power, said secondlens group includes a fourth lens and a fifth lens, said third lensgroup includes a sixth lens having positive refractive power and aseventh lens having negative refractive power, said fourth lens isformed in a meniscus shape so that a concave surface thereof faces theobject side near an optical axis thereof, said first lens has an Abbe'snumber νd1, said second lens has an Abbe's number νd2, said third lenshas an Abbe's number νd3, said sixth lens has an Abbe's number νd6, andsaid seventh lens has an Abbe's number νd7 so that the followingconditional expressions are satisfied:40<νd1<75,20<νd2<35,40<νd3<75,40<νd6<75,20<νd7<35, and said fourth lens has a focal length f4 so that thefollowing conditional expression is satisfied:−15<f4/f<−3 where f is a focal length of a whole lens system.
 2. Theimaging lens according to claim 1, wherein said fourth lens has negativerefractive power, said fifth lens has negative refractive power, andsaid fourth lens has an Abbe's number νd4 and said fifth lens has anAbbe's number νd5 so that the following conditional expressions aresatisfied:20<νd4<3520<νd5<35.
 3. The imaging lens according to claim 1, wherein said fifthlens is disposed away from the sixth lens by a distance D56 on anoptical axis so that the following conditional expression is satisfied:0.02<D56/f<0.15.
 4. The imaging lens according to claim 1, wherein saidfirst lens, said second lens, and said third lens have a composite focallength f123 so that the following conditional expression is satisfied:0.6<f123/f<1.2.
 5. The imaging lens according to claim 1, wherein saidsixth lens and said seventh lens have a composite focal length f67 sothat the following conditional expression is satisfied:−15<f67/f<−1.5.
 6. The imaging lens according to claim 1, wherein saidfourth lens and said fifth lens have a composite focal length f45, andsaid sixth lens has a focal length f6 so that the following conditionalexpression is satisfied:−2<f45/f6<−0.1.
 7. An imaging lens comprising: a first lens group havingpositive refractive power; a second lens group having negativerefractive power; and a third lens group having negative refractivepower, arranged in this order from an object side to an image planeside, wherein said first lens group includes a first lens havingpositive refractive power, a second lens having negative refractivepower, and a third lens having positive refractive power, said secondlens group includes a fourth lens and a fifth lens, said third lensgroup includes a sixth lens having positive refractive power and aseventh lens having negative refractive power, said third lens is formedin a meniscus shape so that a convex surface thereof faces the objectside near an optical axis thereof, said fourth lens is formed in ameniscus shape so that a concave surface thereof faces the object sidenear an optical axis thereof, and said first lens has an Abbe's numberνd1, said second lens has an Abbe's number νd2, said third lens has anAbbe's number νd3, said sixth lens has an Abbe's number νd6, and saidseventh lens has an Abbe's number νd7 so that the following conditionalexpressions are satisfied:40<νd1<75,20<νd2<35,40<νd3<75,40<νd6<75,20<νd7<35.
 8. The imaging lens according to claim 7, wherein said fourthlens has negative refractive power, said fifth lens has negativerefractive power, and said fourth lens has an Abbe's number νd4 and saidfifth lens has an Abbe's number νd5 so that the following conditionalexpressions are satisfied:20<νd4<3520<νd5<35.
 9. The imaging lens according to claim 7, wherein said fifthlens is disposed away from the sixth lens by a distance D56 on anoptical axis so that the following conditional expression is satisfied:0.02<D56/f<0.15 where f is a focal length of a whole lens system. 10.The imaging lens according to claim 7, wherein said first lens, saidsecond lens, and said third lens have a composite focal length f123 sothat the following conditional expression is satisfied:0.6<f123/f<1.2 where f is a focal length of a whole lens system.
 11. Theimaging lens according to claim 7, wherein said sixth lens and saidseventh lens have a composite focal length f67 so that the followingconditional expression is satisfied:−15<f67/f<−1.5 where f is a focal length of a whole lens system.
 12. Theimaging lens according to claim 7, wherein said fourth lens and saidfifth lens have a composite focal length f45, and said sixth lens has afocal length f6 so that the following conditional expression issatisfied:−2<f45/f6<−0.1.
 13. The imaging lens according to claim 7, wherein saidfourth lens has a focal length f4 so that the following conditionalexpression is satisfied:−15<f4/f<−3 where f is a focal length of a whole lens system.
 14. Animaging lens comprising: a first lens group having positive refractivepower; a second lens group having negative refractive power; and a thirdlens group having negative refractive power, arranged in this order froman object side to an image plane side, wherein said first lens groupincludes a first lens having positive refractive power, a second lenshaving negative refractive power, and a third lens having positiverefractive power, said second lens group includes a fourth lens and afifth lens, said third lens group includes a sixth lens having positiverefractive power and a seventh lens having negative refractive power,said third lens is formed in a meniscus shape so that a convex surfacethereof faces the object side near an optical axis thereof, said firstlens has an Abbe's number νd1, said second lens has an Abbe's numberνd2, said third lens has an Abbe's number νd3, said sixth lens has anAbbe's number νd6, and said seventh lens has an Abbe's number νd7 sothat the following conditional expressions are satisfied:40<νd1<75,20<νd2<35,40<νd3<75,40<νd6<75,20<νd7<35, and said fifth lens is disposed away from the sixth lens by adistance D56 on an optical axis so that the following conditionalexpression is satisfied:0.02<D56/f<0.15 where f is a focal length of a whole lens system. 15.The imaging lens according to claim 14, wherein said fourth lens hasnegative refractive power, said fifth lens has negative refractivepower, and said fourth lens has an Abbe's number νd4 and said fifth lenshas an Abbe's number νd5 so that the following conditional expressionsare satisfied:20<νd4<3520<νd5<35.
 16. The imaging lens according to claim 14, wherein saidfirst lens, said second lens, and said third lens have a composite focallength f123 so that the following conditional expression is satisfied:0.6<f123/f<1.2.
 17. The imaging lens according to claim 14, wherein saidsixth lens and said seventh lens have a composite focal length f67 sothat the following conditional expression is satisfied:−15<f67/f<−1.5.
 18. The imaging lens according to claim 14, wherein saidfourth lens and said fifth lens have a composite focal length f45, andsaid sixth lens has a focal length f6 so that the following conditionalexpression is satisfied:−2<f45/f6<−0.1.
 19. The imaging lens according to claim 14, wherein saidfourth lens has a focal length f4 so that the following conditionalexpression is satisfied:−15<f4/f<−3.